Real Riemannian Gaussian Flow Of A Lagrangian, Part 1

 Over the course of any one particular given arbitrary iteration of instanton, at the proximal local covariant locus, of a given arbitrary Noether-Based increment of a discrete energy quantum, let's suppose here, that one were to make a Laplacian-Based tracing, -- from the general covariant locus, of the directly associated holonomic substrate, of the directly corresponding phenomenology of discrete energy impedance, towards, the general covariant locus, of the directly associated holonomic substrate, of the directly corresponding phenomenology of discrete energy permittivity, to where this general flow of a mappable-tracing, will tend to be situated, in a manner that is to be analogous, to the relative forward-holomorphic direction, (as this may be described of here, as being in the "positive i" direction.) Next; Over the course of any one particular given arbitrary iteration of instanton, at the proximal local covariant locus, of a given arbitrary Noether-Based discrete increment of energy quanta, let's suppose that one were to make a Laplacian-Based tracing, -- from the general covariant locus, of the directly associated holonomic substrate, of the directly corresponding phenomenology of discrete energy permittivity, towards, the general covariant locus, of the directly associated holonomic substrate, of the directly corresponding phenomenology of discrete energy impedance, this general flow of a mappable-tracing, tends to be situated, in a manner, that is here to be analogous, to the relative reverse-holomorphic direction, (as this may be described of here, as being in the "negative i" direction.) When one is to make a discrete tense of a coupling, between the "thrust," of a theoretically pure heuristic holomorphic driven tense, of discrete energy permittivity, with the "lag," of a theoretically pure heuristic holomorphic driven tense, of discrete energy impedance, this will consequently tend to work to form the resultant, of a purely unitary flow, in the directly correlative motion, or Lagrangian, of such an inferred discrete quantum of energy. TO BE CONTINUED! SAM.(1989).